Finally, in Fig. REF  we compare the twist-3 GPDs at two different values of \(t\)  with their twist-2 counterparts calculated in Ref. [1]}. For the case of \(\widetilde{H}+\widetilde{G}_2\)  we also compare with their forward limit, \(g_T\) , which we calculated in a separate work [2]}. The setup corresponds to \(P_3=1.25\)  GeV and \(\xi =0\) . We can note that \(g_T(x)\)  is the dominant distribution in magnitude, while \({\widetilde{H}} + {\widetilde{G}_2}\)  is similar in magnitude to \({\widetilde{H}}\)  at \(t=-0.69\)  GeV\(^2\) . Our preliminary results show a mild dependence on \(t\)  for both \({\widetilde{H}} + {\widetilde{G}_2}\)  and \({\widetilde{E}} + {\widetilde{G}_1}\) .
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